H
h2ouniverse
Guest
1) indeed omega is not the same in both diagrams; this is to illustrate the parallel between both problems, not to claim full identity; this is fully exact in the "relative rotation" case; and an analogy in the "relative translation" case. But...<br />2) D is an equivalent distance equal to square root of Izz/m for the rotation case. D=R for a cylinder or a ring. But for a homogeneous sphere D=Rsqrt(2/5). It represents the RMS average of distance between the elementary masses constituting the object and the axis of rotation. It is a measure of the spatial distribution of the object's mass. The analogy I propose to better feel the issues is to consider a "D" for the other pb by positing D=I(u,u')/m, with u and u' the two directions of spacetime about which the "rotation" occurs; I(u,u') would be a momentum of inertia. For rotation in first case that is in plane x,y and the complementary directions are u=z, u'=ct. For the translation case this is in plane x, ct so u=y and u'=z. <br />Note that such D has a real physical meaning in relativity context. Imagine your object is a ring of radius R and axis z. Then D=R. But to stop the motion of such object you need to influence the matter of the ring, commanding from the center. In relativity theory, this cannot occur before a minimum time that is propagation of your actuation at best at speed c. And this minimum time to reach the matter of your object is t1 = D/c. So D represents also the height of the causality cone in the x, ct diagram. Your action to merge the two referentials in the "relative translation" diagram cannot occur in effect before time t1, that is a spacetime distance of ct1 = D! So you can measure the "alpha" angle both and consider the D-radiused circle. For a non-cylindrical object, D and t1 represent RMS averages. Using t1 to normalize t leads to consider ratios t/t1 = ct/D.<br />3) in your example, you do not show one translation and one rotation but two rotations that are fully identical in nature, with